CN201765403U - Device for realizing optical isolation in optical experiment and optical fiber communication system - Google Patents

Device for realizing optical isolation in optical experiment and optical fiber communication system Download PDF

Info

Publication number
CN201765403U
CN201765403U CN2010202267777U CN201020226777U CN201765403U CN 201765403 U CN201765403 U CN 201765403U CN 2010202267777 U CN2010202267777 U CN 2010202267777U CN 201020226777 U CN201020226777 U CN 201020226777U CN 201765403 U CN201765403 U CN 201765403U
Authority
CN
China
Prior art keywords
faraday
optical
high reflectance
reflecting body
wave plate
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN2010202267777U
Other languages
Chinese (zh)
Inventor
底楠
赵建林
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Northwestern Polytechnical University
Original Assignee
Northwestern Polytechnical University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Northwestern Polytechnical University filed Critical Northwestern Polytechnical University
Priority to CN2010202267777U priority Critical patent/CN201765403U/en
Application granted granted Critical
Publication of CN201765403U publication Critical patent/CN201765403U/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Abstract

The utility model relates to a device for realizing optical isolation in an optical experiment and an optical fiber communication system. The device is characterized in that: a positive light polarization state control assembly, an isolation assembly and a negative light polarization state control assembly are sequentially arranged along an optical axis; the positive light polarization state control assembly comprises a first linear polarizer and a first 1/4 wave plate which are sequentially arranged along the optical axis; the isolation assembly comprises a first high-reflectivity reflector, a Faraday rotator and a second high-reflectivity reflector which are sequentially arranged along the optical axis and placed in an axial magnetic field; and the negative light polarization state control assembly comprises a second linear polarizer and a second 1/4 wave plate which are sequentially arranged along the optical axis. The device has the advantages of: effectively reducing the requirement on the temperature stability of the Faraday magneto-optical materials so that the device can be used in a system with large temperature difference environment; realizing the requirement on the isolation degree over 40-65 dB only by utilizing single-stage isolation; and realizing the miniaturization of the parts as the light ray does not displace transversely.

Description

A kind ofly in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device
Technical field
The utility model relates to a kind of optoisolated device of realizing in Experiments of Optics and optical fiber telecommunications system, be used to prevent that the light beam that light source sends from returning light source again behind a certain optical element end face reflection, can be applicable to belong to laser, technical field of optical fiber communication in Experiments of Optics and the optical fiber telecommunications system.
Background technology
In systems such as Experiments of Optics and optical fiber communication, the light beam that luminescent device sends can be caused influences such as light source video stretching, noise increase, power shakiness, performance degradation by the end face reflection of a certain optical element of downstream light path and back light source again.In order to protect luminescent devices such as laser instrument, image intensifer, eliminate the reflecting light of not expecting, guarantee system stable operation, often need in the light path of light source output terminal back, place a kind of optical device that allows the light one-way transmission, be referred to as optoisolator usually.
Optoisolator can be divided into two classes by polarization characteristic, i.e. polarization relationship type and polarization independent type.Existing polarization relationship type optoisolator is mainly formed (referring to Fig. 1) by the polarizer, Faraday polarization apparatus and analyzer, the direction of shaking the thoroughly angle at 45 of shake the thoroughly direction and the polarizer of analyzer, and Faraday polarization apparatus places between the two.Incident light becomes linearly polarized light after by the polarizer, through thoroughly the shake direction rotation 45 ° of its plane of polarization behind the Faraday polarization apparatus to analyzer, just in time is parallel to the direction of shaking thoroughly of analyzer, thereby can passes through analyzer smoothly again; Emergent light is reverse through analyzer and Faraday polarization apparatus by the end face part of optical element in the light path of downstream reflection back, because the Faraday effect of Faraday polarization apparatus, the reflected light plane of polarization is vertical with the polarizer direction of shaking thoroughly along continuing 45 ° of rotations with the direction of the identical rotation direction of incident light polarization face, thereby make light beam can't oppositely pass through the polarizer, realize isolation effect.Because Faraday polarization apparatus is relevant with the temperature of plane polarization light wavelength and this device environment of living in to the angle of linearly polarized light rotation, therefore, this type of optoisolator can only be realized above-mentioned functions usually in less relatively temperature range.
Polarization independent type optical isolator mainly contains two kinds of displacement type and wedge shapes.Its ultimate principle is, between two GRIN Lens, place a polarizing beam splitter, two orthogonal polarization components (being o light and the e light in the uniaxial crystal) of incident beam are made apart, the light beam that forward passes through synthesizes a branch of light again at another polarizing beam splitter place behind Faraday polarization apparatus, and can not synthesize a branch of light again behind the light beam that oppositely passes through process polarizing beam splitter and the Faraday polarization apparatus, thereby realize isolation effect.Yet, have only when two reverse cross polarization light components in the space separately more greatly apart from the time, just can play buffer action, this makes and to need large-size as the crystal of polarizing beam splitter and faraday rotator or birefringent wedge crystal, thereby causes the volume of device big, cost is high.
Summary of the invention
The technical matters that solves
For fear of the deficiencies in the prior art part, the utility model proposes a kind of optoisolated device of in Experiments of Optics and optical fiber telecommunications system, realizing, overcome the existing narrower deficiency of isolator operating temperature range, satisfy the requirement of device miniaturization simultaneously, this optoisolator can be realized the function of logical light of forward and reverse isolation in a wider temperature range, and realizes satisfying the requirement of device miniaturization.
Technical scheme
A kind ofly in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device, it is characterized in that comprising forward polarization state Control Component 1, barrier assembly 2 and the negative polarization state Control Component of establishing along the optical axis order 3; First linear polarizer 11 and first quarter-wave plate 12 of described forward polarization state Control Component 1 for establishing, and the direction of shaking the thoroughly angle at 45 of the quick shaft direction of first quarter-wave plate 12 and first linear polarizer 11 along the optical axis order; Described barrier assembly 2 comprises Faraday polarization apparatus 21, the first high reflectance reflecting body 22, the second high reflectance reflecting body 23, anti-reflection film 24, micro-displacement apparatus 25, permanent magnet 26 and supporter 41; At the two ends of supporter 41 fixed permanent magnet 26 and micro-displacement apparatus 25, the centre of permanent magnet 26 is a Faraday polarization apparatus 21, and the both sides of Faraday polarization apparatus (21) are the first high reflectance reflecting body 22 and anti-reflection film 24; Micro-displacement apparatus 25 and anti-reflection film 24 close ends are provided with the second high reflectance reflecting body 23; Faraday polarization apparatus 21, the first high reflectance reflecting body 22, the second high reflectance reflecting body 23 and anti-reflection film 24 are same optical axis; Second linear polarizer 31 and second quarter-wave plate 32 of described negative polarization state Control Component 3 for establishing along the optical axis order, the quick shaft direction of second quarter-wave plate 32 is parallel with the quick shaft direction of first quarter-wave plate 12, and the direction of shaking thoroughly of second linear polarizer 31 is vertical with the direction of shaking thoroughly of first linear polarizer 11.
When the quick shaft direction of the quick shaft direction of described second quarter-wave plate 32 and first quarter-wave plate 12 was vertical, the direction of shaking thoroughly of second linear polarizer 31 was parallel with the direction of shaking thoroughly of first linear polarizer 11.
The described first high reflectance reflecting body 22 and the second high reflectance reflecting body 23 are catoptron or reflectance coating, and reflectivity is more than 80%, preferred 92%.
Described Faraday polarization apparatus 21 is made of the magneto-optic memory technique of the parallel polishing of both ends of the surface that produces Faraday effect, and described magneto-optic memory technique is that faraday's anglec of rotation that the magneto-optical crystal of yttrium iron garnet YIG, terbium gallium garnet TGG, contour Fil moral constant or magneto-optic thin film, requirement produce is 15 °~75 °.
Described axial magnetic field 27 is one to be applied to the permanent magnet 26 on the Faraday polarization apparatus 21; Described permanent magnet 26 is neodymium iron boron Nd-Fe-B or SmCo Sm-Co.
Described anti-reflection film 24 is monofilm or assembly of thin films.
Described micro-displacement apparatus 25 is piezoelectric chip PZT.
Faraday's anglec of rotation of described Faraday polarization apparatus (21) is 45 °.
Principle of work of the present utility model: after first linear polarizer is passed in the forward entrance monochromatic light incident that laser instrument sends, become the monochromatic linearly polarized light of forward; Shake thoroughly behind first quarter-wave plate at direction angle at 45 through quick shaft direction and first linear polarizer again, become forward monochrome circularly polarized light; Then normal incidence is to containing in Fabry-Perot etalon Faraday polarization apparatus, that be made of the first high reflectance reflecting body and the second high reflectance reflecting body.The refractive index of the monochromatic circularly polarized light of described forward in Faraday polarization apparatus is N 1This Fabry-Perot etalon chamber length is a desired value, can make the monochromatic circularly polarized light of described forward is the integral multiple of π by the first high reflectance reflecting body through the one way phase shift of Faraday polarization apparatus to the second high reflectance reflecting body, form the multiple beam constructive interference, then this Fabry-Perot etalon has the largest light intensity transmitance to the monochromatic circularly polarized light of forward, and the monochromatic circularly polarized light of forward passes through this Fabry-Perot etalon with high permeability.Afterwards, the monochromatic circularly polarized light of forward becomes and the consistent linearly polarized light of initial incident forward monochrome plane polarization light polarization direction after by perpendicular second quarter-wave plate of quick shaft direction and first quarter-wave plate, and pass outgoing behind the direction of shaking second linear polarizer consistent, thereby realize the logical light function of forward of optoisolator with this plane polarization light polarization direction.
Emergent light is returned along original optical path is reverse by reflecting body end face part reflection back in the light path of downstream, is converted into behind second linear polarizer and second quarter-wave plate and the opposite reverse monochromatic circularly polarized light in the monochromatic circularly polarized light polarization direction of forward; Then normal incidence is in the described Fabry-Perot etalon that contains Faraday polarization apparatus.Faraday polarization apparatus has different refractive indexes to the light of different rotation directions, and the refractive index of reverse monochromatic circularly polarized light in Faraday polarization apparatus is N 2Therefore, under the length of the above-mentioned suitable chamber of Fabry-Perot etalon, reverse monochromatic circularly polarized light is the odd-multiple of pi/2 by the second high reflectance reflecting body through the one way phase shift of Faraday polarization apparatus to the first high reflectance reflecting body, can form the multiple beam destructive interference, this Fabry-Perot etalon has the minimum intensity of light transmitance to reverse monochromatic circularly polarized light, and reverse monochromatic circularly polarized light passes through this Fabry-Perot etalon with low transmission, thereby realizes the reverse isolation function of optoisolator.
Beneficial effect
The optoisolated device of realization in Experiments of Optics and optical fiber telecommunications system that the utility model proposes, beneficial effect is: utilize compression and the filter action to spectrum of the nonreciprocal effect of the left and right sides rounding polarized light characteristic that refractive index is different in the Faraday magneto-optical material, Faraday effect and Fabry-Perot etalon, the Faraday magneto-optical material is placed in the Fabry-Perot etalon, realization has high permeability and the circularly polarized light of another opposite rotation direction is had the effect of low transmission the circularly polarized light of a certain rotation direction, reaches optoisolated purpose.
Advantage is:
1, the utility model utilizes Faraday effect to control the effect of the phase differential realization light isolation of generation pi/2 between the circularly polarized light of opposite rotation direction, therefore but do not need faraday's rotation angle strict and steady on 45 °, promptly, the small size variation of faraday's rotation angle is the serious performance of deterioration optoisolator not, effectively reduce requirement like this, therefore can be used for being operated in the system of big temperature difference environment Faraday magneto-optical material temperature stability;
2, only utilize single-stage to isolate the requirement that just can realize the above isolation of 40-65dB;
3, light does not produce transversal displacement, can realize miniaturization of devices.
Description of drawings
Fig. 1 realizes optoisolated apparatus structure synoptic diagram;
Fig. 2 is the transmittance curve comparison diagram of different rotation direction circularly polarized lights when utilizing the utility model to realize isolation; Solid line be under the different condition light positive to by the time transmittance curve; Dotted line be under the corresponding conditions light oppositely by the time transmittance curve;
Fig. 3 utilizes the utility model to realize that isolation time strong reflection rate R and faraday's rotation angle θ are to isolation influence curve comparison diagram.
Among the figure, 1-forward polarization state Control Component, 11-first linear polarizer, 12-first quarter-wave plate; The 2-barrier assembly, 21-Faraday polarization apparatus, the 22-first high reflectance reflecting body, the 23-second high reflectance reflecting body, 24-anti-reflection film, 25-micro-displacement apparatus, 26-permanent magnet, 27-axial magnetic field; 3-negative polarization state Control Component, 31-second linear polarizer, 32-second quarter-wave plate; The 41-supporter, 42-first optical fiber collimator, 43-incident optical, 44-second optical fiber collimator, 45-outgoing optical fiber, 46-sleeve, 47-laser instrument, 48-reflecting body.
Embodiment
Now in conjunction with the embodiments, accompanying drawing is further described the utility model:
See also Fig. 1, present embodiment is applied to comprise laser instrument 47, first linear polarizer 11, first quarter-wave plate 12, Faraday polarization apparatus 21, the first high reflectance reflecting body 22, anti-reflection film 24, permanent magnet 26, the second high reflectance reflecting body 23, micro-displacement apparatus 25, supporter 41, second quarter-wave plate 32, second linear polarizer 31 and reflecting body 48 in the Experiments of Optics system that resolution element builds.Faraday polarization apparatus 21 places the inside of permanent magnet 26, its magneto-optic memory technique is selected yttrium iron garnet crystal (YIG) for use, its on forward entrance light direction end face, be coated with reflectivity be 92% reflectance coating as the first high reflectance reflecting body 22, it is coated with anti-reflection film 24 on forward emergent light direction end face; The second high reflectance reflecting body 23 is positioned at after the Faraday polarization apparatus 21, links with micro-displacement apparatus 25, and constitutes Fabry-Perot etalons, Faraday polarization apparatus 21 parallel this etalons that are positioned at the first high reflectance reflecting body 22; Micro-displacement apparatus 25, Faraday polarization apparatus 21 and permanent magnet 26 overall fixed are on supporter 41.First linear polarizer 11 and first quarter-wave plate 12 are parallel successively to be positioned at before the described Fabry-Perot etalon, and the quick shaft direction angle at 45 of shake the thoroughly direction and first quarter-wave plate 12 of first linear polarizer 11; Second quarter-wave plate 32 and second linear polarizer 31 are parallel successively to be positioned at after the described Fabry-Perot etalon, and the quick shaft direction of second quarter-wave plate 32 is vertical with the quick shaft direction of first quarter-wave plate 12, and the direction of shaking thoroughly of second linear polarizer 31 is parallel with the direction of shaking thoroughly of first linear polarizer 11.Anti-reflection film 24 reduces the monofilm or the assembly of thin films of reflection, enhancing transmission for making incident light at the interface.Permanent magnet 26 is the permanent magnet of a hollow drum NdFeB material, and it is parallel to even axial magnetic field optical direction, that the magnetic field positive dirction is identical with the forward entrance light direction for Faraday polarization apparatus 21 provides.Micro-displacement apparatus 25 is piezoelectric chip (PZT), can make by its adjustment to contain Fabry-Perot etalon Faraday polarization apparatus 21, that constitute by the first high reflectance reflecting body 22 and the second high reflectance reflecting body 23 to have an optimum chamber long, to obtain the optimal isolation degree.
The course of work of present embodiment is: in coordinate system as shown in Figure 4, the forward entrance light that laser instrument 47 sends is to be converted into the forward linearly polarized light that the polarization direction is x-y plane one or three quadrant angle bisectors behind first linear polarizer 11 of x-y plane one or three quadrant angle bisectors to the direction of shaking thoroughly along z axle positive dirction vertical incidence, again through too fast axle for be converted into forward right-circularly polarized light (this rotation direction goes into to define in face of described) behind axial first quarter-wave plate 12 of y when light is observed.The refractive index of described forward right-circularly polarized light in Faraday polarization apparatus 21 is n -, its light intensity transmitance of passing through behind the Fabry-Perot etalon that contains Faraday polarization apparatus 21 that is made of the first high reflectance reflecting body 22 and the second high reflectance reflecting body 23 is
T = 1 1 + 4 R ( 1 - R ) 2 sin 2 ( φ - )
In the formula, R is the light intensity reflectivity of the first high reflectance reflecting body 22 and the second high reflectance reflecting body 23, φ -For described forward right-circularly polarized light by of the one way phase shift of the first high reflectance reflecting body 22 through Faraday polarization apparatus 21 to second high reflectance reflecting bodys 23.By moving the micro-displacement apparatus 25 that links with the second high reflectance reflecting body 23, adjust φ -Be the integral multiple of π, make the forward right-circularly polarized light form the complete constructive interference of multiple beam in the Fabry-Perot etalon that contains Faraday polarization apparatus 21, this moment, light intensity transmitance T was a maximal value, realized the purpose of the logical light of forward.The forward right-circularly polarized light is converted into the forward linearly polarized light that the polarization direction is x-y plane one or three quadrant angle bisectors again after too fast axle is for axial second quarter-wave plate 32 of x, be similarly lossless ejaculation behind second linear polarizer 31 of x-y plane one or three quadrant angle bisectors through the direction of shaking thoroughly, become the forward emergent light.
Described forward emergent light is returned along z axle negative direction by the end face part of reflecting body 48 in the light path of downstream reflection back, reverse vertical incident is converted into the reverse linearly polarized light that the polarization direction is x-y plane one or three quadrant angle bisectors after passing second linear polarizer 31 that the direction of shaking is x-y plane one or three quadrant angle bisectors, is to be converted into the reverse right-circularly polarized light opposite with forward right-hand circular polarization light polarization direction when described backlight is observed (this rotation direction in face of definition) behind second quarter-wave plate 32 of x axle through quick shaft direction again.The refractive index of described reverse right-circularly polarized light in Faraday polarization apparatus 21 is n +, its light intensity transmitance of passing through behind the Fabry-Perot etalon that contains Faraday polarization apparatus 21 that is made of the first high reflectance reflecting body 22 and the second high reflectance reflecting body 23 is
T = 1 1 + 4 R ( 1 - R ) 2 sin 2 ( φ + )
In the formula, φ +For described reverse right-circularly polarized light by of the one way phase shift of the second high reflectance reflecting body 23 through Faraday polarization apparatus 21 to first high reflectance reflecting bodys 22.Because Faraday polarization apparatus 21 couples of little refractive index differences, i.e. n in the Fabry-Perot etalon with the rotation direction circularly polarized light -With n +Unequal, so forward right-circularly polarized light and reverse right-circularly polarized light have different one way phase shifts after by same Faraday polarization apparatus 21, its difference is
Δφ = | φ + - φ - | = 2 π | n + - n - | L λ = 2 θ = 2 VBL
In the formula, L is the logical light length of Faraday magneto-optical material, and V is the Fil moral constant of Faraday magneto-optical material, and θ is faraday's rotation angle, and B is the magnetic field that is applied on the Faraday polarization apparatus 21.By regulating the size control faraday rotation angle θ of magnetic field β, can adjust the one way phase shift difference of different rotation direction circularly polarized lights, when θ=45 °, described one way phase shift difference Δ φ=pi/2, this moment is as forward right-circularly polarized light one way phase shift φ -Be the integral multiple of π, form the multiple beam constructive interference, when having the largest light intensity transmitance, the one way phase shift φ of reverse right-circularly polarized light +Be the odd-multiple of pi/2, form the multiple beam destructive interference, have the minimum intensity of light transmitance, realize the purpose of reverse isolation.
The effect of described Faraday polarization apparatus 21 is to make the phase differential that produces pi/2 between the circularly polarized light of opposite rotation direction,, makes forward right-circularly polarized light one way phase shift φ that is -For the integral multiple of π forms complete constructive interference, reverse right-circularly polarized light one way phase shift φ +For the odd-multiple of pi/2 forms complete destructive interference; Faraday's rotation angle θ of the generation of its generation is as the criterion so that different rotation direction circularly polarized lights can effectively be separated the transmittance curve spike of Fabry-Perot etalon, usually be limited between 15 °-75 °, then isolation effect is good more near 45 ° more, and optimal value is 45 ° (referring to Fig. 2 and Fig. 3).
The light intensity reflectivity R of the described first high reflectance reflecting body 22 and the second high reflectance reflecting body 23 is limited in more than 80% usually, bigger R helps the increase of isolation, but the requirement to later stage device assembling and mechanical stability is higher, otherwise, less R is unfavorable for the realization of high-isolation, but can reduce the requirement to later stage device assembling and mechanical stability; Preferred 92% (referring to Fig. 2 and the Fig. 3) of light intensity reflectivity R.

Claims (9)

1. in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device for one kind, it is characterized in that comprising forward polarization state Control Component (1), barrier assembly (2) and the negative polarization state Control Component of establishing along the optical axis order (3); First linear polarizer (11) and first quarter-wave plate (12) of described forward polarization state Control Component (1) for establishing, and the direction of shaking the thoroughly angle at 45 of the quick shaft direction of first quarter-wave plate (12) and first linear polarizer (11) along the optical axis order; Described barrier assembly (2) comprises Faraday polarization apparatus (21), the first high reflectance reflecting body (22), the second high reflectance reflecting body (23), anti-reflection film (24), micro-displacement apparatus (25), permanent magnet (26) and supporter (41); At the two ends fixed permanent magnet (26) and the micro-displacement apparatus (25) of supporter (41), the centre of permanent magnet (26) is Faraday polarization apparatus (21), and the both sides of Faraday polarization apparatus (21) are the first high reflectance reflecting body (22) and anti-reflection film (24); The end that micro-displacement apparatus (25) is close with anti-reflection film (24) is provided with the second high reflectance reflecting body (23); Faraday polarization apparatus (21), the first high reflectance reflecting body (22), the second high reflectance reflecting body (23) and anti-reflection film (24) are same optical axis; Second linear polarizer (31) and second quarter-wave plate (32) of described negative polarization state Control Component (3) for establishing along the optical axis order, the quick shaft direction of second quarter-wave plate (32) is parallel with the quick shaft direction of first quarter-wave plate (12), and the direction of shaking thoroughly of second linear polarizer (31) is vertical with the direction of shaking thoroughly of first linear polarizer (11).
2. according to claim 1ly in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device, it is characterized in that: when the quick shaft direction of the quick shaft direction of described second quarter-wave plate (32) and first quarter-wave plate (12) was vertical, the direction of shaking thoroughly of second linear polarizer (31) was parallel with the direction of shaking thoroughly of first linear polarizer (11).
3. according to claim 1ly in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device, it is characterized in that: the described first high reflectance reflecting body (22) and the second high reflectance reflecting body (23) are catoptron or reflectance coating, and reflectivity is more than 80%.
4. according to claim 1ly in Experiments of Optics and optical fiber telecommunications system, realize optoisolated device, it is characterized in that: described Faraday polarization apparatus (21) is made of the magneto-optic memory technique of the parallel polishing of both ends of the surface that produces Faraday effect, and described magneto-optic memory technique is that faraday's anglec of rotation that the magneto-optical crystal of yttrium iron garnet YIG, terbium gallium garnet TGG, contour Fil moral constant or magneto-optic thin film, requirement produce is 15 °-75 °.
5. according to claim 1ly realize optoisolated device in Experiments of Optics and optical fiber telecommunications system, it is characterized in that: described axial magnetic field (27) is one to be applied to the permanent magnet (26) on the Faraday polarization apparatus (21); Described permanent magnet (26) is neodymium iron boron Nd-Fe-B or SmCo Sm-Co.
6. isolation device according to claim 1 is characterized in that: described anti-reflection film (24) is monofilm or assembly of thin films.
7. isolation device according to claim 1 is characterized in that: described micro-displacement apparatus (25) is piezoelectric chip PZT.
8. isolation device according to claim 4 is characterized in that: faraday's anglec of rotation of described Faraday polarization apparatus (21) is 45 °.
9. isolation device according to claim 3 is characterized in that: described reflectivity is 92%.
CN2010202267777U 2010-06-17 2010-06-17 Device for realizing optical isolation in optical experiment and optical fiber communication system Expired - Fee Related CN201765403U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2010202267777U CN201765403U (en) 2010-06-17 2010-06-17 Device for realizing optical isolation in optical experiment and optical fiber communication system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2010202267777U CN201765403U (en) 2010-06-17 2010-06-17 Device for realizing optical isolation in optical experiment and optical fiber communication system

Publications (1)

Publication Number Publication Date
CN201765403U true CN201765403U (en) 2011-03-16

Family

ID=43718011

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2010202267777U Expired - Fee Related CN201765403U (en) 2010-06-17 2010-06-17 Device for realizing optical isolation in optical experiment and optical fiber communication system

Country Status (1)

Country Link
CN (1) CN201765403U (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101872077A (en) * 2010-06-17 2010-10-27 西北工业大学 Optoisolator for use in fiber-optic communication
CN101872076A (en) * 2010-06-17 2010-10-27 西北工业大学 Optical experiment and method for implementing optical isolation in optical fiber communication system and device thereof
CN106773148A (en) * 2016-12-21 2017-05-31 中国科学院福建物质结构研究所 Optical isolator and method
CN114967187A (en) * 2022-05-26 2022-08-30 北京航空航天大学 Free space optical isolator

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101872077A (en) * 2010-06-17 2010-10-27 西北工业大学 Optoisolator for use in fiber-optic communication
CN101872076A (en) * 2010-06-17 2010-10-27 西北工业大学 Optical experiment and method for implementing optical isolation in optical fiber communication system and device thereof
CN101872076B (en) * 2010-06-17 2012-09-26 西北工业大学 Optical experiment and method for implementing optical isolation in optical fiber communication system and device thereof
CN101872077B (en) * 2010-06-17 2012-11-21 西北工业大学 Optoisolator for use in fiber-optic communication
CN106773148A (en) * 2016-12-21 2017-05-31 中国科学院福建物质结构研究所 Optical isolator and method
CN106773148B (en) * 2016-12-21 2019-07-30 中国科学院福建物质结构研究所 Optical isolator and method
CN114967187A (en) * 2022-05-26 2022-08-30 北京航空航天大学 Free space optical isolator

Similar Documents

Publication Publication Date Title
CN101872076B (en) Optical experiment and method for implementing optical isolation in optical fiber communication system and device thereof
US20140300963A1 (en) Optical Isolator
EP0391703A2 (en) Quasi-achromatic optical isolators and circulators using prisms with total internal fresnel reflection
US20230296930A1 (en) Single and multi-stage high power optical isolators using a single polarizing element
CN201765403U (en) Device for realizing optical isolation in optical experiment and optical fiber communication system
CN109001864A (en) Optoisolator and semiconductor laser elements
CN101872077B (en) Optoisolator for use in fiber-optic communication
CN201698114U (en) Device for realizing optical isolation
US6278547B1 (en) Polarization insensitive faraday attenuator
CN201859277U (en) Optical isolator for fiber-optic communication
US10962813B2 (en) Optical isolator module
JP2542532B2 (en) Method for manufacturing polarization-independent optical isolator
US20030184861A1 (en) Optical isolator
WO2003032055A1 (en) Reflective variable light attenuator
JP2006208948A (en) Variable optical attenuator
US6384957B1 (en) Variable optical attenuator utilizing Faraday effect
JPH0244310A (en) Optical isolator
JP4794056B2 (en) Optical device
GB2143337A (en) Optical isolator
US9791627B1 (en) Integrated optical components with wavelength tuning and power isolation functions
JP2565423B2 (en) Optical isolator
JP2004177639A (en) Reflective variable magneto-optical device
JPS61132925A (en) Semiconductor laser module with optical isolator
JP2005265901A (en) Optical component
JPH04264515A (en) Optical isolator

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20110316

Termination date: 20130617